Magnetic processing of electronic materials

ABSTRACT

The electronic properties (such as electron mobility, resistivity, etc.) of an electronic material can be modified/enhanced when subjected to dynamic or stationary magnetic fields in conjunction with select cycles of heating, cooling and passage of electric current through the material. This “processing” includes one or more cycles using combinations of the aforementioned variables.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims priority of U.S. provisional patent Application No. 60/573,994, filed May 24, 2004 and entitled “Magnetic Pumping Effects on Electronic Materials.”

SUMMARY

The electronic properties (such as electron mobility, resistivity, etc.) of an electronic material can be modified/enhanced when subjected to dynamic or stationary magnetic fields in conjunction with select cycles of heating, cooling and passage of electric current through the material. This “processing” includes one or more cycles using combinations of the aforementioned variables.

BRIEF DESCRIPTION OF THE DRAWINGS

The features, aspects, and advantages of the invention will become more thoroughly apparent from the following detailed description, appended claims, and accompanying drawings in which:

FIG. 1 illustrates a layout of an n-type/p-type thermoelectric generator with two magnets.

FIG. 2 illustrates a magnet “movement” for processing on electronic material.

FIG. 3 is a simplified side view of a “magnetic belt” for processing an electronic material.

FIG. 4 is a simplified top plan view of the magnetic belt shown in FIG. 3.

FIG. 5 is a simplified top plan view of an alternative arrangement of a magnetic belt.

FIGS. 6A-6B are simplified top plan views of further alternative arrangements of a magnetic belt.

FIG. 7 illustrates a rotational processing configuration.

FIGS. 8A-8C illustrate processing of a rod-shaped workpiece.

FIG. 9 illustrates processing of a plate-shaped workpiece.

DETAILED DESCRIPTION

Electronic materials have so far been assigned typical physical output values that have been determined by testing. Most of these test values have been taken in a standard ambient environment and, to date, the effects of subjecting the materials to other enhancing environments have not been studied. This invention relates to techniques for enhancing the performance of electronic materials by subjecting them to magnetic fields.

The electronic properties (such as electron mobility, resistivity, etc.) of an electronic material can be modified/enhanced when subjected to dynamic or stationary magnetic fields in conjunction with select cycles of heating, cooling and passage of electric current through the material. This “processing” includes one or more cycles using combinations of the aforementioned variables.

This process can be used in-situ with products such as photovoltaics, thermoelectric electric generation, thermoelectric cooling, detectors, transistors, etc. It could also be used to improve material/device performance prior to installation in electronic assemblies. Further, either the magnetic fields or the material/device (or both) could be dynamic. The magnetic field combinations that can be used are boundless. However, it should be noted that the magnetic fields used are directional and not oscillatory.

Preliminary testing of magnetic fields on electronic materials has been conducted as follows:

-   -   1) A thermoelectric generator was set up and heated to T1 in a         closed environment (FIG. 1).     -   2) Airflow was introduced on the cool side of the generator to         maximize the temperature difference and current. The heavy         airflow also eliminated any cooling by below magnet movements.     -   3) After an hour of working the current flow had stabilized to a         value of I₀.     -   4) Magnetic flux was applied, 50 elliptical “movements” (FIG. 2)         at approximately 1 Hz, to both n and p parts of the         thermoelectric generator; current value was recorded at 1.6×I₀.     -   5) The thermoelectric generator was cooled down to room         temperature.     -   6) The thermoelectric generator was reheated to T1 and allowed         to stabilize with the same airflow for an hour; the new current         was recorded at 1.25×I₀.     -   7) A stationary magnetic field was applied to the TE generator         and current was recorded at 1.4×I₀.     -   8) The thermoelectric generator was cooled down to room         temperature.     -   9) After cool down, reheating to T1, providing airflow and         stabilizing, a magnetic flux was applied, 100 “movements” at         approximately 1 Hz, to both n and p parts of the thermoelectric         generator, current value was recorded at 1.95×I₀.     -   10) After cool down, reheating to T1, providing airflow and         stabilizing the new current draw was recorded at >1.3×I₀.     -   11) A stationary magnetic field was applied to the         thermoelectric generator and current was recorded at ≈1.5×I₀.     -   12) Procedures 1-11 were repeated several times with the same         outcome.

It should be noted that higher frequency (greater than the 1 Hz used in preliminary testing) and infinite/continuous movements (circular/elliptical/oscillated motion at the side of or around the electronic material) of the magnet(s) are each expected to have a positive impact on performance enhancement for electronic materials.

For the above-described preliminary testing, the following new physical effects were observed:

-   -   1) magnetic “quenching/tempering” of electronic materials, prior         to their use, enhances the materials performance;     -   2) using a quenched electronic material with a magnetic field         (in certain applications) further enhances performance of the         material; and     -   3) applying magnetic flux to a working electronic material         creates a pumping effect on the workings of the material which         multiplies the output several times.

In summary, the magnetic quenching/tempering for each electronic material may include a specific process with controlled combinations of the following:

-   -   1) setup for electronic material     -   2) temperature     -   3) rate of heat up     -   4) magnetic field strength     -   5) magnetic flux/frequency (possibly determined by material's         natural frequency)     -   6) movement of magnets     -   7) number of cycles used by magnets     -   8) time for magnetic flux application     -   9) rate of cool down     -   10) number of times above cycles 1 to 8 are performed.

Thus, many ingots/rods of electronic materials could be magnetically quenched/tempered to inexpensively achieve much better output performance.

Dynamic or “staggered” magnetic fields may be used to create a more powerful pumping action on the electronic material. The following testing performed by the inventor demonstrated that controlled magnetic flux can produce pumping action to increase the current flowing in an electronic material by varying the pattern and frequency of the magnetic flux applied to the electronic material:

-   -   1) A magnetically quenched (annealed) n-p thermoelectric module         was set up and heated to temperature T1 in a closed environment.     -   2) Airflow was introduced on the cool side of the thermoelectric         module to maximize the temperature difference and current. The         airflow also eliminated any cooling by below magnet movements.     -   3) After the current flow had stabilized in the module, the         current value was recorded at I_(A).     -   4) Unidirectional dynamic magnetic flux was applied to both n         and p parts of the annealed thermoelectric module using a         “standard magnetic belt” (i.e., magnets 10 attached to a belt 20         as in FIG. 3) with a magnet pattern as shown in FIG. 4. The new         current value was recorded at 1.5×I_(A).     -   5) The same unidirectional dynamic magnetic flux was applied to         only the n-part of the thermoelectric module. The new current         value was recorded at approximately 1.1×I_(A).     -   6) The thermoelectric module was cooled to room temperature.     -   7) Next, after cool down, reheating to T1, providing airflow and         stabilizing the annealed thermoelectric module, the stabilized         current was recorded the same, i.e., I_(A).     -   8) The same unidirectional dynamic magnetic flux was once again         applied to both n and p parts of the annealed thermoelectric         module using a different “staggered magnetic belt” with a         pattern as shown in FIG. 5. The new current value was recorded         at approximately 1.30×I_(A).

The following additional testing was also performed:

-   -   after cool down, reheating to T1, providing airflow and         stabilizing the annealed thermoelectric module, the stabilized         current was recorded at I_(A).     -   unidirectional dynamic magnetic flux was applied to both n and p         parts of the annealed thermoelectric module using the “standard         magnetic belt.” The current value was recorded at 1.15×I_(A).     -   the magnetic belt movement was then reversed and it was observed         that the current dropped to zero. The current stayed at zero         until the original “correct” magnetic belt movement was         restored; the current then shot back at 1.15×I_(A).     -   The magnetic belt movement was once again reversed and it was         observed once again that the current dropped to zero. This time         the magnetic belt was then moved away from the thermoelectric         module and it was observed the current stayed at zero for a long         time before it very slowly began to creep upwards.

From the above testing, the following new additional physical effects were observed:

-   -   1) applying a directional staggered dynamic magnetic flux to an         electronic material provides a pumping action to the charges in         the current, similar to a paddle wheel on a river boat, that         produces a turbocharged enhancement to the electronic material         performance;     -   2) reversing the direction of the dynamic magnetic flux to an         electronic material produces an abrupt, immediate braking action         to performance of the material; this effect can be made to stay         continuous or temporary;     -   3) applying magnetic flux to a working electronic material         creates a pumping effect on the workings of the material which         multiplies the output several times.

The following should be noted:

-   -   dynamic magnetic cycling can also be accomplished with the use         of electromagnets, but these are expensive and use a lot of         electricity;     -   the above testing can be performed with many other magnet cycle         combinations; a few are illustrated in FIGS. 6A and 6B;     -   to obtain optimum results for each specific application,         polarity of each magnetic flux applied can be modified by         design; and     -   the magnetic belts may include a variety of designs, such as the         magnets could be on the inside or outside of the belt, the belt         is circulated around the electronic material, the belt is         circulated between two electronic materials, etc.

Thus, the performance of many electronic products can be further improved during operation, beyond magnetic annealing, with the application of dynamic magnetic flux, standard or staggered. In addition, the new unique effect discovered (of immediate zero current with reverse dynamic magnetic flux) will provide many new, more reliable “braking” applications for electronic materials, such as precision brakes for automobiles, emergency shutdown for electronic equipment, etc.

FIG. 7 illustrates a processing configuration comprising a drive shaft 30 connected to a motor 40. The shaft is supported with two wheels 50 mounted on the shaft, each wheel loaded with several powerful rare-earth magnets 60 mounted around the circumference of each wheel. Most of the major components are of non-magnetic materials to avoid affecting the magnetic fields' performance.

An electronic workpiece is introduced in a mold (not depicted) between the wheels. The material is heated or cooled with optional electric current applied. The motor is turned on and the rotating magnets produce pulsed, directional dynamic magnet fields on the workpiece.

As previously discussed, the frequency and configurations of the magnets used will depend on the material and electronic property selected for modification/improvement.

Note that this process is not restricted only to small parts or devices, nor limited by the number of “wheels” or number/type/orientation of magnets used in the process. FIGS. 8 and 9 provide conceptual design of the means to perform similar applications to large workpieces.

FIG. 8 provides details of use with a large electronic rod 70. The magnets surround the workpiece and are attached to the inside of a cylinder. Successive magnet layers, along the workpiece, can be modified to produce turbulent magnetic actions on the workpiece. Either the cylinder with magnets or the workpiece may be rotated.

FIG. 9 provides another use for a flat sheet or plate 80. Magnets 90 are attached to belts 100 and the belts are cycled around the workpiece.

Processing in accordance with the present invention is not limited to semiconductor materials; it may also be used for so-called “standard” electronic materials, such as metallic wire, foil conductors, etc. For example, the application of dynamic magnetic fields in an electric motor or alternator/generator may be used to enhance output/performance.

In certain cases, it may be beneficial to skew the position of the magnets so that they are at an acute angle to either of the major axes (i.e., x-y-z) relative to the workpiece. The resulting “screw type” action (or paddle wheel effect) of the magnetic fields will further accelerate the moving charges, of the applied/existing current in the workpiece, along the length of the workpiece thereby enhancing the charge flow in the workpiece. 

1. A method of treating an electronic material comprising: configuring the electronic material to carry an electrical current; applying a time-varying unidirectional magnetic field to the electronic material.
 2. The method of claim 1 further comprising heating the electronic material to an elevated temperature prior to applying the time-varying unidirectional magnetic field.
 3. The method of claim 1 wherein the time-varying unidirectional magnetic field is generated by orbital motion of a magnet.
 4. The method of claim 1 wherein the time-varying unidirectional magnetic field is generated by linear movement of a magnet. 